GCM activities in Ulrike Lohmann’s group

Slides:



Advertisements
Similar presentations
© Crown copyright Met Office Cloudier Evaluating a new GCM prognostic cloud scheme using CRM data Cyril Morcrette, Reading University, 19 February 2008.
Advertisements

Robin Hogan (with input from Anthony Illingworth, Keith Shine, Tony Slingo and Richard Allan) Clouds and climate.
Evaluation of ECHAM5 General Circulation Model using ISCCP simulator Swati Gehlot & Johannes Quaas Max-Planck-Institut für Meteorologie Hamburg, Germany.
By : Kerwyn Texeira. Outline Definitions Introduction Model Description Model Evaluation The effect of dust nuclei on cloud coverage Conclusion Questions.
IACETH Institute for Atmospheric and Climate Science Boundary Layer parametrisation in the climate model ECHAM5-HAM Colombe Siegenthaler - Le Drian, Peter.
A cloud scheme including indirect aerosol effects on ice and liquid cloud particles in the MRI Earth System Model SAKAMI, T., T.OSE and S. YUKIMOTO with.
Uintah Basin WRF Testing Erik Neemann 20 Sep 2013.
Test simulation of Aerosol impact on solar radiation with WRF-CHEM DustDNI (w/o dust) – DNI (w/ dust) Positive value indicates the decreased DNI due to.
Aerosol effect on cloud cover and cloud height Kaufman, Koren, Remer, Rosenfeld & Martins.
Radiative Properties of Eastern Pacific Stratocumulus Clouds Zack Pecenak Evan Greer Changfu Li.
Evaluation of CMIP5 Simulated Clouds and TOA Radiation Budgets in the SMLs Using NASA Satellite Observations Erica K. Dolinar Xiquan Dong and Baike Xi.
Influences of In-cloud Scavenging Parameterizations on Aerosol Concentrations and Deposition in the ECHAM5-HAM GCM Betty Croft - Dalhousie University,
Aerosol-Cloud Interactions and Radiative Forcing: Modeling and Observations Graham Feingold 1, K. S. Schmidt 2, H. Jiang 3, P. Zuidema 4, H. Xue 5, P.
Morrison/Gettelman/GhanAMWG January 2007 Two-moment Stratiform Cloud Microphysics & Cloud-aerosol Interactions in CAM H. Morrison, A. Gettelman (NCAR),
Aerosol Size-Dependent Impaction Scavenging in Warm, Mixed, and Ice Clouds in the ECHAM5-HAM GCM Betty Croft, and Randall V. Martin – Dalhousie University,
Betty Croft, and Randall V. Martin – Dalhousie University, Canada
Boundary Layer Clouds.
Influences of In-cloud Scavenging and Cloud Processing on Aerosol Concentrations in ECHAM5-HAM Betty Croft - Dalhousie University, Halifax, Canada Ulrike.
A study of ice formation by primary nucleation and ice multiplication in shallow precipitating embedded convection T. Choularton 1, I. Crawford 1, C. Dearden.
IACETH Institute for Atmospheric and Climate Science Cirrus Clouds triggered by Radiation Fabian Fusina ETH - Zurich 1 st EULAG Workshop - 9th October.
Representation of Subgrid Cloud-Radiation Interaction and its Impact on Global Climate Simulations Xinzhong Liang (Illinois State Water Survey, UIUC )
Yuqing Wang and Chunxi Zhang International Pacific Research Center University of Hawaii at Manoa, Honolulu, Hawaii.
Reasoning for Microphysics Modifications -Several modification were made to Thompson microphysics schemes: -Changes to homogeneous freezing temperature.
Application of Ice Microphysics to CAM Xiaohong Liu, S. J. Ghan (Pacific Northwest National Laboratory) M. Wang, J. E. Penner (University of Michigan)
Uintah Basin WRF Testing Erik Neemann 20 Sep 2013.
Update on progress with the implementation of a new two-moment microphysics scheme: Model description and single-column tests Hugh Morrison, Andrew Gettelman,
The Third Indirect Aerosol-Cloud Effect: Global Model Sensitivity and Restrictions Hans-F. Graf and Frank J. Nober EGS-AGU-ESF meeting Nice, April 2003.
Parameterization of cloud droplet formation and autoconversion in large-scale models Wei-Chun Hsieh Advisor: Athanasios Nenes 10,Nov 2006 EAS Graduate.
COPE PRESENTATION Process Modeling and Ice Nuclei.
Approach We use a model of intermediate complexity and a fully Bayesian statistical model to update over time the PDF of ECS as we incorporate increasingly.
Status of CAM, March 2004 Phil Rasch. Differences between CAM2 and CAM3 (standard physics version) Separate liquid and ice phases Advection, sedimentation.
Two Frigid 2014 Snow Storms – A Look at Snow to Liquid Ratios
15th Annual CMAS Conference
Putting the Clouds Back in Aerosol-Cloud Interactions
Environmental Physics Laboratory, Institute of Physics Belgrade
EASC 11 Clouds and Precipitation
Tests with Liu-Penner ice microphysics in Hirlam Karl-Ivar-Ivarsson, Aladin/ Hirlam all staff meeting Krakow April
Review for Exam 2 Fall 2011 Topics on exam: Class Lectures:
Investigating Cloud Inhomogeneity using CRM simulations.
Ice Microphysics in CAM
Advisors: Fuqing Zhang and Eugene Clothiaux
Clouds and Large Model Grid Boxes
H. Morrison, A. Gettelman (NCAR) , S. Ghan (PNL)
Simulation of the Arctic Mixed-Phase Clouds
What are the causes of GCM biases in cloud, aerosol, and radiative properties over the Southern Ocean? How can the representation of different processes.
OBR: Cloud Physics Research
Relationships inferred from AIRS-CALIPSO synergy
5. Formation and Growth of Ice Crystals
The representation of ice hydrometeors in ECHAM-HAM
Understanding warm rain formation using CloudSat and the A-Train
Cloud Types and Precipitation
Improvement of Cloud Cover Fraction parameterization in Chemistry Transport Model(CTM) Zhenzhen Yin.
Atmospheric Modeling and Analysis Division,
Pre-industrial and historical simulations with MPI-ESM-HAM
Microphysical-macrophysical interactions or Why microphysics matters
Influences of Wet Scavenging on Aerosol Concentrations and Deposition in the ECHAM5-HAM Global Climate Model Betty Croft1 Ulrike.
Constraining the aerosol indirect effect
Evolution of tropical cirrus clouds.
John Marsham and Steven Dobbie
A. Gettelman, X. Liu, H. Morrison, S. Ghan
Assessment of NASA GISS CMIP5 and post-CMIP5 Simulated Clouds and Radiation fluxes Using Satellite Observations 1/15/2019 Ryan Stanfield(1), Xiquan Dong(1),
CO2 forcing induces semi-direct effects
Short Term forecasts along the GCSS Pacific Cross-section: Evaluating new Parameterizations in the Community Atmospheric Model Cécile Hannay, Dave Williamson,
The radiative properties of inhomogeneous cirrus clouds
Effects of 3D radiation on cloud evolution
Application of Stochastic Techniques to the ARM Cloud-Radiation Parameterization Problem Dana Veron, Jaclyn Secora, Mike Foster, Christopher Weaver, and.
Review of Roesenfeld et al
Presented as Discussion Material for the Radiative Coupling Project
Humidity.
Climatic implications of changes in O3
Presentation transcript:

GCM activities in Ulrike Lohmann’s group With results from Remo Dietlicher, David Neubauer and Steffen Münch

Gradual improvements in ECHAM-HAM Activation scheme Cloud cover scheme Convective detrainment Accretion of ice by snow Cirrus ice crystal number Mixed-phase freezing ECHAM5.5-HAM2.0 (E55H20): Zhang et al. (2012) ECHAM6.1-HAM2.2 (E61H22): Neubauer et al. (2014) ECHAM6.3-HAM2.3 (E63H23): Tegen et al. (2018)

Gradual improvements in ECHAM-HAM More cloud water in stratocumulus regions and less elsewhere

Gradual improvements in ECHAM-HAM Generally, newer model versions are better Improvements are gradual

Cloud formation processes in a prognostic cloud cover scheme (Steffen Münch)

Cloud cover sources

Ice crystal sources

Cloud type contributions to the LW and SW cloud radiative effects in REF and Steffen’s model Make clearer that this is a pathway analysis Warm liquid raus

Most of the mixed-phase temperature regime is covered by ice that formed below -35 °C Make clearer that this is a pathway analysis Warm liquid raus Homogeneous freezing at temperatures colder than -35 °C dominates mixed-phase ice (Dietlicher et al. 2018, ACPD)

Cloud radiative effects per formation pathway Process rates Formation pathways Model integration Cloud fields Formation pathways keep track of the relative contribution of each process rate to the simulated cloud fields.

Supercooled liquid fraction (SLF) Obs. ECHAM also underestimates SLF, but less than CESM  do we also underestimate ECS? And if so, by how much? CESM Figure from Tan et al. (2016), ECHAM results from Lohmann and Neubauer (2014)

Equilibrium climate sensitivity CESM ECHAM6-HAM2 No ECS shift from cloud phase feedback between simulation REF and ALL_LIQ in ECHAM6-HAM2 despite a smaller negative cloud phase feedback in ALL_LIQ because of compensating feedbacks in the clear-sky CESM Figure from Tan et al. (2016)

Impact of Remo’s new ice microphysics scheme But: with our new ice microphysics scheme (Dietlicher et al., ACPD, 2018 and in prep.) the cloud optical depth feedback becomes positive and climate sensitivity increases to 3.8 ºC (vs. 2.5 ºC in REF)

Take-home messages – modelling results We have two new stratiform cloud schemes: The single-category ice microphysics scheme of Remo (Dietlicher et al., ACPD, 2018) and a new cloud cover scheme also with changed microphysics from Steffen. Both schemes are more physical and perform at least as well as our current scheme. The supercooled liquid fraction is not a good indicator for the cloud phase feedback because cloud phase matters most for clouds not shielded by higher clouds ECS is significantly higher when using the Remo’s ice microphysics scheme with 3.8 ºC vs. 2.5 ºC. The reasons for this require further analysis but could be linked to a smaller contribution of mixed-phase clouds in that scheme.

Sensitivity studies: Which processes are necessary to reproduce the observations? Ice nucleation on dust and vertical cirrus cover both bring the simulated ice crystal number concentration closer to observations. But there are still too many ice crystals in the model (watch out for scale).